线性金属纳米球阵列上的行电磁波

R. Shore, A. Yaghjian
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引用次数: 1

摘要

在最近的一篇报告[1]中,我们采用了带有矢量球形波函数[3]-[4]的源散射矩阵公式[2],研究了无损可穿透(磁介质)球体的无限线性周期阵列上的行电磁波。假设要么球体足够小,只有偶极散射场可以被激发,要么频率足够高,除了偶极场之外,所有散射的多极场都可以忽略不计。因此,仅使用电偶极子和磁偶极子矢量球波来处理球散射,偶极子彼此正交并与阵列轴正交。在最近的一次会议上提出了这项工作的摘要。虽然我们的研究在一定程度上是受到Holloway等人最近的理论论证的推动。该理论证明,通过在背景矩阵中嵌入磁介电球阵列可以形成双负介质,但结果同样适用于无损“金属”球体阵列,具有负的相对介电常数和等于1的相对磁导率,由横向的电磁场激发到阵列轴。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Traveling electromagnetic waves on linear metallic nanosphere arrays
In a recent report [1] we have employed the source scattering-matrix formulation [2] with vector spherical wave functions [3]–[4] to investigate traveling electromagnetic waves on infinite linear periodic arrays of lossless penetrable (magnetodielectric) spheres. It is assumed that either the spheres are sufficiently small that only the dipole scattered fields can be excited, or the frequency is such that all the scattered multipole fields are negligible except the dipole fields. Accordingly, the sphere scattering is treated using only electric and magnetic dipole vector spherical waves, the dipoles being orthogonal to each other and to the array axis. A summary of this work was presented at a recent conference [5]. Although our investigation was motivated in part by the recent theoretical demonstration by Holloway et al. [6] that a doubly negative medium can be formed by embedding an array of magnetodielectric spheres in a background matrix, the results are equally applicable to arrays of lossless “metallic” spheres, with negative relative permittivity and with relative permeability equal to one, excited by an electromagnetic field transverse to the array axis.
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